Issue |
EPL
Volume 95, Number 4, August 2011
|
|
---|---|---|
Article Number | 47008 | |
Number of page(s) | 6 | |
Section | Condensed Matter: Electronic Structure, Electrical, Magnetic and Optical Properties | |
DOI | https://doi.org/10.1209/0295-5075/95/47008 | |
Published online | 27 July 2011 |
Electron pockets and pseudogap Dirac point in underdoped cuprate superconductors
1
Department of Physics, University of Guelph - Guelph, Ontario, Canada N1G 2W1
2
Guelph-Waterloo Physics Institute, University of Guelph - Guelph, Ontario, Canada N1G 2W1
3
Department of Physics and Astronomy, McMaster University - Hamilton, Ontario, Canada L8S 4M1
4
The Canadian Institute for Advanced Research - Toronto, Ontario, Canada M5G 1Z8
Received:
11
May
2011
Accepted:
28
June
2011
We consider a model of the pseudogap specifically designed to describe the underdoped cuprates and which exhibits particle-hole asymmetry. The presence of electron pockets, besides the usual hole pockets, leads to the appearance of new vectors beyond the usual so-called octet model in the joint density of states (JDOS), which underlies the analysis of Fourier-transform scanning tunneling spectroscopy (FT-STS) data. These new vectors are associated with distinct patterns of large amplitude in the JDOS and are expected to occur primarily at positive bias. Likewise a pseudogap Dirac point occurs at positive bias and this point can be determined either through FT-STS or through extrapolation of data from the autocorrelation function of angle-resolved photoemission spectroscopy.
PACS: 74.72.-h – Cuprate superconductors / 74.72.Kf – Pseudogap regime / 74.20.Mn – Nonconventional mechanisms
© EPLA, 2011
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